Polar Oxysulfide for Nonlinear Optical Applications

ABSTRACT

Single crystals of a new noncentrosymmetric polar oxysulfide SrZn 2 S 2 O (s.g. Pmn 2   1 ) grown in a eutectic KF—KCl flux with unusual wurtzite-like slabs consisting of close-packed corrugated double layers of ZnS 3 O tetrahedra vertically separated from each other by Sr atoms and methods of making same.

This invention was made with government support under DE-SC0008664 awarded by the Department of Energy. The government has certain rights in the invention.

BACKGROUND OF THE INVENTION 1) Field of the Invention

The present invention relates to single crystals of a new noncentrosymmetric polar oxysulfide SrZn₂S₂O (s.g. Pmn2₁) grown in a eutectic KF—KCl flux with unusual wurtzite-like slabs consisting of close-packed corrugated double layers of ZnS₃O tetrahedra vertically separated from each other by Sr atoms and methods of making same.

2) Description of Related Art

A number of physical properties, such as piezoelectricity, ferroelectricity, and second harmonic generation (SHG), only occur in materials having noncentrosymmetric (NCS) crystal structures and, as discussed by Halasyamani and Poeppelmeier, specific physical properties require the presence of specific symmetry elements in the structure in order for these properties to exist.

For example, for a material to be ferroelectric it needs to be noncentrosymmetric and polar (a subcategory of NCS structures), while for piezoelectric and SHG behaviors polar symmetry is sufficient, but not required. However, with the exception of the crystal class 432, acentricity is required. All polar structures are noncentrosymmetric, but not all NCS structures are polar. In general, both polar and NCS materials are uncommon as the vast majority of materials crystallize in centrosymmetric structures. A large number of approaches have therefore been pursued to favor the formation of NCS structures, including the synthesis of structures exhibiting second order Jahn-Teller distortions and the use of chiral ligands.

Other approaches have targeted the use of tetrahedral building blocks that can result in a polar crystal structure if all the vertices point in the same direction. This happens in a number of structural families. For example, Ln₃MO₆ (M=Fe and Ga and Ln=Nd, Sm, Eu, and Gd) crystallizes in the polar space group Cmc2₁, in which the vertices line up along the crystallographic and, therefore, polar z-direction. Another popular approach has relied on mixed anion polyhedral building blocks, such as octahedral MF_(6-x)O_(x) and tetrahedral MQ_(4-x)O_(x) (Q=S, Se, and Te) units containing different anions with different charges, sizes, electronegativities, and polarizabilities. In order for such materials to be polar, three conditions must be met: (1) the anions in the polyhedron must be crystallographically ordered (favored by charge and electronegativity differences); (2) the polyhedral orientation must exhibit long-range order; and (3) the polyhedral long-range structure must result in an overall net polarity.

In the case of octahedral MF_(6-x)O_(x) units, the most common metal cations have been Ti, Nb, and Mo, with which wide band gap materials containing MF_(6-x)O_(x) units can readily be formed under mild reaction conditions and where, depending on the value of x, different structural arrangements are possible. In the case of tetrahedral MQ_(4-x)O_(x) units, the most common metals have been M=Zn, V, Fe, Co, Ga, Ge, and, P, where not every value of x is attainable for every element listed. Furthermore, several elements, such as Fe and Co, while present in a number of polar materials, are not appropriate for optical applications due to the fact that the presence of their d-electrons imparts color. One of the most useful elements for optical applications is Zn²⁺ with a d¹⁰ electron configuration, where for oxychalcogenides, large band gap, optically transparent, polar materials have been reported, including BaZnSO, SrZnSO, and CaZnSO. These compositions are related to several iron and cobalt oxychalcogenide phases, CaFeSO, CaCoSO, and CaFe—SeO. The symmetries and tilts of these compositions are quite varied and result in different space groups, for example, BaZnSO (Cmcm), SrZnSO (P6_(3mc)), CaFeSO (P6_(3mc)), CaZnSO (P6_(3mc)), CaFeSeO (Cmc2₁), and CaFeSeO (Pmcn); furthermore, multiple polymorphs can crystallize together.

One decade ago, the SHG properties of two oxysulfides, CaZnSO and α-Na₃PO₃S with highly distorted tetrahedral units, were investigated using 1064 nm radiation by Clarke and Aitken, respectively. These materials exhibited SHG efficiencies 100-200 times that of α-quartz, but nonphase matching behaviors were observed. While phase matchability is a pivotal requisite for making SHG materials practically useful, so far, the relationship between phase matchability and crystal structure of inorganic NCS materials is not well understood.

Given the scarcity of NCS oxysulfide phases, the discovery of new oxysulfides with chemically similar local structures but different degrees or orientations of acentric building units will support the development of the chemical design of new high SHG efficient materials. Accordingly, it is an object of the present disclosure to expand this class of oxychalcogenide materials and synthesize new members of the class.

SUMMARY OF THE INVENTION

The above objectives are accomplished according to the present invention by providing in a first embodiment, a new zinc oxysulfide compound. The compound may be a noncentrosymmetric crystalline structure with chemical formula SrZn₂S₂O, may have lattice parameters of α=3.87440(10) Å, b=9.9847(3) Å, and c=6.0916(2) Å, and may have corrugated double layers of ZnS₃O tetrahedra vertically separated by Sr²⁺ ions. Further, the compound may have an O/S anion ordered arrangement provides two distinct orientations of the ZnS₃O tetrahedra. Still yet, the compound may crystalize in the noncentrosymmetric polar space group Pmn2₁. Still yet, the O/S anion ordered arrangement may yield two distinct orientations of the Zn-centered tetrahedra. Yet further, the compound may form colorless and transparent crystals. Still again, the compound may have a band gap of 3.86 eV. Yet further, the compound may be stable up to 650° C. in O₂ gas atmosphere. Again still, the compound may be phase matchable with twice the SHG intensity of potassium dihydrogen phosphate (KDP). Further again, the compound may have a Sr:Zn:S molar ratio of approximately 1.0:2.0:2.3. Still yet, the compound may have a band gap energy of 3.86 eV. Still further, temperatures greater than 1000° C. may decompose the SrZn₂S₂O compound.

In an alternative embodiment, a method for synthesizing the compound SrZn₂S₂O is provided. The method may include employing a molten salt method using a eutectic KF—KCl mixture, loading a silver tube with 1 mmol of SrO, 1 mmol of Zn, 1 mmol of S, 3.4 mmol of KF, and 4.1 mmol of KCl, placing the silver tube in a silica tube that was evacuated to 10⁻⁴ Pa and sealed, and heating the silver tube in a tube furnace to 900° C. at 5° C./min, held for 24 h, and cooled to 600° C. at 0.17° C./min. Still further, the method may include extracting the compound from flux by dissolving the flux in water and aided by sonication.

In a still further embodiment, a method for solid state synthesis of SrZn₂S₂O is provided. The method may include mixing SRO, Zn and S in a stoichiometric ratio in an agate mortar, pressing the mixture into a pellet, heating the pellet in an evacuated silica tube at 1000° C. for 24 hours, and sonicating at 1000° C. with water.

BRIEF DESCRIPTION OF THE DRAWINGS

The construction designed to carry out the invention will hereinafter be described, together with other features thereof. The invention will be more readily understood from a reading of the following specification and by reference to the accompanying drawings forming a part thereof, wherein an example of the invention is shown and wherein:

FIG. 1 shows Table 1—Results of Structural Refinement of SrZn₂S₂O Using Single-Crystal XRD Data.

FIG. 2 shows Table 2—Selected Interatomic Distances (Å) and Bond Angles (deg) of SrZn₂S₂O at Room Temperature.

FIG. 3 shows at (a, b) a perspective view of the SrZn₂S₂O crystal structure along the a and c axes and at (c) O/S anion-ordered arrangement in the close-packed layers of ZnS₃O tetrahedra.

FIG. 4 shows the local coordination environment around Sr and Zn atoms.

FIG. 5 shows a thermogravimetric curve of SrZn₂S₂O in O₂ gas atmosphere.

FIG. 6 shows the UV-vis-NIR optical absorption spectrum of SrZn₂S₂O.

FIG. 7 shows at (a) total and partial density of states and at (b) band dispersions of SrZn₂S₂O.

FIG. 8 shows SHG intensities of SrZn₂S₂O and KDP are plotted against particle size.

FIG. 9 shows Table 3—Direction and Magnitude of the Dipole Moments (in Debye) of the Polyhedral Building Units in SrZn₂S₂O, CaZnSO, and Wurtzite ZnS.

FIG. 10 shows a photograph of a colorless transparent single crystal of SrZn₂S₂O.

FIG. 11 shows a comparison of the powder XRD pattern of purified SrZn₂S₂O with a theoretical pattern based on the single-crystal XRD analysis.

FIG. 12 shows SXRD patterns for purified SrZn₂S₂O measured at room temperature.

FIG. 13 shows a room-temperature XRD pattern of the products after TG measurement.

FIG. 14 shows a comparison of the crystal structure of SrZn₂S₂O (Pmn2₁) with that of CaFeSeO (C_(mc)2₁).

FIG. 15 shows Crystal Orbital Hamiltonian Population (COHP) for (Zn1/Zn2)-O and (Zn1/Zn2)-S interactions in SrZn₂S₂O.

FIG. 16 shows Table 4—Atomic coordinates and equivalent isotropic displacement parameters Ueq for SrZn₂S₂O at 300 K.

FIG. 17 shows Table 5—Anisotropic displacement parameters U_(ij) (10²×Å²) for SrZn₂S₂O at 300 K.

FIG. 18 shows Table 6—Lattice constants and atomic coordinates obtained by the first principle calculations for SrZn₂S₂O

FIG. 19 shows Table 7—Atomic coordinates and isotropic displacement parameters Biso refined from SXRD data collected from SrZn₂S₂O at room temperature.

It will be understood by those skilled in the art that one or more aspects of this invention can meet certain objectives, while one or more other aspects can meet certain other objectives. Each objective may not apply equally, in all its respects, to every aspect of this invention. As such, the preceding objects can be viewed in the alternative with respect to any one aspect of this invention. These and other objects and features of the invention will become more fully apparent when the following detailed description is read in conjunction with the accompanying figures and examples. However, it is to be understood that both the foregoing summary of the invention and the following detailed description are of a preferred embodiment and not restrictive of the invention or other alternate embodiments of the invention. In particular, while the invention is described herein with reference to a number of specific embodiments, it will be appreciated that the description is illustrative of the invention and is not constructed as limiting of the invention. Various modifications and applications may occur to those who are skilled in the art, without departing from the spirit and the scope of the invention, as described by the appended claims. Likewise, other objects, features, benefits and advantages of the present invention will be apparent from this summary and certain embodiments described below, and will be readily apparent to those skilled in the art. Such objects, features, benefits and advantages will be apparent from the above in conjunction with the accompanying examples, data, figures and all reasonable inferences to be drawn therefrom, alone or with consideration of the references incorporated herein.

DETAILED DESCRIPTION OF A PREFERRED EMBODIMENT

With reference to the drawings, the invention will now be described in more detail. Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood to one of ordinary skill in the art to which the presently disclosed subject matter belongs. Although any methods, devices, and materials similar or equivalent to those described herein can be used in the practice or testing of the presently disclosed subject matter, representative methods, devices, and materials are herein described.

Unless specifically stated, terms and phrases used in this document, and variations thereof, unless otherwise expressly stated, should be construed as open ended as opposed to limiting. Likewise, a group of items linked with the conjunction “and” should not be read as requiring that each and every one of those items be present in the grouping, but rather should be read as “and/or” unless expressly stated otherwise. Similarly, a group of items linked with the conjunction “or” should not be read as requiring mutual exclusivity among that group, but rather should also be read as “and/or” unless expressly stated otherwise.

Furthermore, although items, elements or components of the disclosure may be described or claimed in the singular, the plural is contemplated to be within the scope thereof unless limitation to the singular is explicitly stated. The presence of broadening words and phrases such as “one or more,” “at least,” “but not limited to” or other like phrases in some instances shall not be read to mean that the narrower case is intended or required in instances where such broadening phrases may be absent.

The current disclosure focused on the Sr—Zn—S—O system and synthesized the new composition, SrZn₂S₂O, crystallizing in the polar space group Pmn2₁. SrZn₂S₂O is compositionally, but not structurally, related to SrFe₂S₂O and SrFe₂Se₂O, which crystallize in the centrosymmetric space group Pmmn. The current disclosure provides the synthesis, crystal structure, and SHG behavior of this new polar oxysulfide material.

Single crystals of a new zinc oxysulfide SrZn₂S₂O were grown in a eutectic KF—KCl flux, and the structure was determined by single-crystal X-ray diffraction. SrZn₂S₂O crystallizes in the noncentrosymmetric polar space group Pmn2₁ with lattice parameters of α=3.87440(10) Å, b=9.9847(3) Å, and c=6.0916(2) Å. In the crystal structure, close-packed corrugated double layers of ZnS₃O tetrahedra, which are derived from the wurtzite structure, are vertically separated by Sr²⁺ ions. In addition, the O/S anion ordered arrangement in each close-packed layer yields two distinct orientations of the Zn-centered tetrahedra. The crystals of SrZn₂S₂O are colorless and transparent, and the oxysulfide has a band gap of 3.86 eV, based on UV-vis-NIR diffuse reflectance measurements. Thermogravimetric measurements showed that SrZn₂S₂O is stable up to 650° C. in O₂ gas atmosphere. First-principle calculations indicate that the valence band maximum is mainly composed of O-2p and S-3p states, whereas the conduction band minimum is derived from Zn-4s, Zn-4p, and Sr-4d states. The calculated band dispersion reveals a direct band gap corresponding to a transition between S-3p and Zn-4s energy levels. Second harmonic generation (SHG) measurements determined that SrZn₂S₂O is phase matchable with twice the SHG intensity of potassium dihydrogen phosphate (KDP) in contrast to CaZnSO with similar ZnS₃O building units, which exhibits non-phase matching behavior.

Experimental Section

Reagents.

Zn (Alpha Aesar, 99.9%) and S (Fisher, 99.99%) in powder form were used as received. SrO was prepared by heating SrCO₃ in air at 1050° C. overnight. KF (Alpha Aesar, 99.9%) and KCl (Alpha Aesar, 99.9%) were dried at 260° C. prior to use.

Crystal Growth.

Single crystals of SrZn₂S₂O were obtained by a molten salt method using a eutectic KF—KCl mixture. A silver tube welded closed on one end was loaded with 1 mmol of SrO, 1 mmol of Zn, 1 mmol of S, 3.4 mmol of KF, and 4.1 mmol of KCl. The top of the tube was crimped, and the tube was placed inside a silica tube that was evacuated to 10⁻⁴ Pa and sealed. The starting materials were heated in a tube furnace to 900° C. at 5° C./min, held for 24 h, and cooled to 600° C. at 0.17° C./min at which point the furnace was turned off and allowed to cool to room temperature. The product was extracted from the flux by dissolving the flux in water, aided by sonication. Colorless transparent plate-like crystals of SrZn₂S₂O (typical dimension 0.1×0.2×0.05 mm³, see FIG. 10) were isolated via vacuum filtration. Semiquantitative analyses by energy-dispersive X-ray analysis (EDS) indicated a Sr:Zn:S molar ratio of approximately 1.0:2.0:2.3. The structure of SrZn₂S₂O was solved by single crystal X-ray diffraction.

Solid-State Synthesis.

Polycrystalline powder samples of SrZn₂S₂O were synthesized using SrO, Zn, and S in a stoichiometric ratio. The starting materials were thoroughly mixed in an agate mortar, pressed into a pellet, and heated in an evacuated silica tube at 1000° C. for 24 h. Powder XRD measurement using a Bruker D2 Phaser equipped with an LYNXEYE silicon strip detector and a Cu Kα source identified SrZn₂S₂O as the main phase and SrS as a minor phase. Additional heat treatment under the same condition did not improve the relative amount of SrZn₂S₂O to SrS. Heating at higher temperatures (>1000° C.) decomposed SrZn₂S₂O. A pure sample was obtained by sonicating the product prepared at 1000° C. with water in which SrS readily decomposes and the remaining SrZn₂S₂O was isolated by vacuum filtration. The powder XRD data of SrZn₂S₂O after removal of SrS is shown in FIG. 11. A Rietveld refinement of the synchrotron powder XRD data of SrZn₂S₂O after removal of SrS is shown in FIG. 12, and the atomic coordinates and atomic displacement parameters are listed in FIG. 19, which shows Table 7—Atomic coordinates and isotropic displacement parameters Biso refined from SXRD data collected from SrZn₂S₂O at room temperature. The space group is Pmn21 (No. 31) with α=3.87466(1) Å, b=9.98582 Å, and c=6.09207 Å. R indices are Rwp=2.44%, Rp=1.65%, RB=7.129%, and RF=5.47%. Site occupancy for each atom was fixed to unity. The Biso parameters for S1 and S2 were constrained to the same value during refinements. The c coordinate of Sr atom (the heaviest element) along the polar axis was fixed to those obtained by the single-crystal structure analysis.

Single Crystal Structure Determination.

X-ray intensity data were collected from a clear colorless crystal using a Bruker D8 QUEST diffractometer. The D8 utilizes an Incoatec microfocus source (Mo Kα radiation, λ=0.71073 Å) and a Photon II CMOS area detector. The detector was operated in the shutterless mode, and fast scans with 1 s exposure times were used to quantify peaks that were too intense for the detector to measure during the full data collection. Data collection covered 98.8% of reciprocal space up to θ_(max)=36.308°, with an average redundancy of 15. The raw area detector frames were reduced and corrected for Lorentz, polarization, and absorption effects using the SAINT+ and SADABS programs. Initial structural models and subsequent least-squares refinements were performed with the SHELX package, through the OLEX² GUI.

The title compound crystallizes in the NCS orthorhombic space group Pmn2₁ with lattice parameters α=3.87440(10) Å, b=9.9847(3) Å, and c=6.0916(2) Å. The asymmetric unit contains one Sr site, two Zn sites, two S sites, and one O site, all of which lie on Wyckoff site 2a with mirror symmetry. Each site was individually allowed to freely refine, and there were no significant deviations from unity. PLATON modules TwinRotMat and Addsym were used to check for minor twin components and missed symmetry elements. The twin law (−1 0 0 0 −1 0 0 0 −1) with volume fraction 0.032(6) was implemented, and the model was refined as a two-component inversion twin. No missed symmetry elements were found, confirming the NCS space group. The final refinement based on the model resulted in an excellent Ri value of 0.0133 and the small maximum, and minimum residual electron densities of 1.109 and −0.758 indicate an excellent fit of the model to the data.

Powder XRD, TGA, and UV-Vis.

Powder X-ray diffraction (PXRD) patterns were collected at room temperature using a Bruker D2 Phaser instrument. Patterns were collected in the 5-65° 2θ angular range with a step size of 0.02°. Thermogravimetric analysis (TGA) was performed using a PerkinElmer Pyris 1 TGA system under O₂ gas flow (60 mL/min). The sample was loaded in an alumina crucible and heated to 1000° C. at 10° C./min. The thermal products were analyzed by PXRD. UV-vis-NIR absorption measurements on SrZn₂S₂O were carried out using a Shimazu UV2600 UV-vis-NIR spectrometer (used in the diffuse reflectance mode) equipped with an integrating sphere. Deuterium and halogen lamps were used as sources of UV and visible-NIR light, respectively. Spectra were recorded over the range of 220-1200 nm. The diffuse reflectance data were converted to absorbance internally by the instrument by use of the Kubelka-Munk function.

SHG Measurements.

The powder SHG measurements were carried out with the Kurtz-Perry method using a pulsed Nd:YAG Quantel Ultra laser (Model: Ultra 50) with a wavelength of 1064 nm. KH₂PO₄ (KDP) was used as a benchmark material. SrZn₂S₂O and KDP were ground and sieved into distinct particle size ranges (<20, 20-45, 45-63, 63-75, 75-90, 90-125 μm). The intensities of the frequency-doubled output emitted from the sieved samples were detected using a photomultiplier tube and recorded on the Tektronix oscilloscope (Model: TDS3032).

Density Functional Theory (DFT) Calculations.

First-principles DFT calculations were performed for SrZn₂S₂O using the Vienna Ab Initio Simulation Package. The Perdew-Burke-Ernzerchof generalized gradient approximation (GGA) was employed for the exchange and correlation function. Projector augmented-wave potentials were used for Sr, Zn, S, and O atoms. The cell parameters and atomic positions were optimized until the maximum force on each atom was less than 0.02 eV/Å, based on the experimentally determined crystal structure. Then, a single point calculation was carried out to calculate a band structure and density of states. Plane wave basis sets with a cutoff of 500 and 520 eV were used for the optimization and single point calculations, respectively. In both calculations, the self-consistent field tolerance was 1.0×10⁻⁷ eV/atom and the k-point mesh was 9×5×7. The crystal orbital Hamilton population (COHP) analysis was performed using the LOBSTER code.

Results and Discussion

The single-crystal structure solution established that SrZn₂S₂O crystallizes in the NCS polar space group of Pmn2₁ (No. 31). The details of the structural refinement are listed in Table 1, selected interatomic distances and angles are compiled in Table 2, and atomic coordinates and atomic displacement parameters are listed in Tables 4 and 5.

SrZn₂S₂O crystallizes in a unique two-dimensional structure, shown in FIG. 3, in which wurtzite-like slabs, consisting of close-packed corrugated double layers of ZnS₃O tetrahedra, are located in the ac plane. The slabs are separated from each other vertically by Sr²⁺ ions positioned parallel to the ac plane. The O²⁻ and S²⁻ ions, both of which occupy two inequivalent crystallographic positions, are crystallographically ordered and located in each layer such that the oxide ions are connected to both electropositive Sr²⁺ and electropositive Zn²⁺ ions. Furthermore, the ZnS³O tetrahedra have two distinct orientations in the ab plane and are connected by a common shared sulfur apex that creates the corrugation. This type of layered structure is substantially different from other wurtziterelated intergrowth structures, where the corner-shared tetrahedra form single layers of MS₃O (M=Fe, Co, Zn) tetrahedra in which all tetrahedra have the same orientation.

The heteroleptic zinc coordination environment creates the asymmetric tetrahedral coordination, as illustrated in FIG. 4. The Zn(1)-O and Zn(2)-O bond distances of 1.9196(17) A and 1.9468(19) Å, respectively, are somewhat longer than the Zn-O bond distances in CaZnSO (1.8997(5) Å) and SrZnSO (1.9000(7) Å) having similar Zn-centered coordination, but are shorter by 2-3% than the average Zn-O bond distance of 1.979 Å in wurtzite ZnO. The Zn(1)-S(2) and Zn(2)-S(1) bond distances are similar to the Zn—S bond distances found in CaZnSO (2.3718(5) Å) and SrZnSO (2.4173(9) Å) and are longer by 1.4 and 2.5%, respectively, than the average Zn—S bond distance of 2.343 Å in wurtzite ZnS. The Zn(1)-S(1) and Zn(2)-S(2) bond distances are within 1% of the distances observed in wurtzite. The bond angles of O—Zn—S and S—Zn—S are within ±4% of the ideal value (109.5°) for a regular tetrahedron. The Sr²⁺ ions are found in a distorted octahedral coordination environment consisting of two oxide ions at 2.3985(10) Å and four sulfide ions at 3.0087(8)-3.1102(8) Å, yielding a second asymmetric unit in the structure. The bond-valence-sum (BVS) calculations resulted in 2.02 for Sr, 1.99 for Zn(1), and 1.90 for Zn(2), which are in good agreement with the expected oxidation states.

The long-range order and coexistence of mixed anions in the same layer in SrZn₂S₂O are quite unique because, typically, oxygen and the other chalcogens tend to be separated in different layers. Recently, similar anion order in a different framework was reported for the iron-based oxychalcogenides, AFe₂Q₂O (A=Sr, Ba; Q=S, Se) and CaFeSeO. In the structure of AFe₂Q₂O two infinite chains of FeQ₃O tetrahedra share oxygen apexes to create double chains, which in turn are connected by sharing three sulfur atoms with another double chain, resulting in layers. These close packed layers are stacked parallel with A²⁺ layers perpendicular to the hexagonal c-axis, unlike SrZn₂S₂O, where the layers are parallel to the hexagonal c-axis. Another example is CaFeSeO, crystallizing in the space group Cmc2₁ which can be considered to be a member of a homologous series (AO)(MQ)n (M=Fe, Zn; n=1, 2) to which CaFeSeO and SrZn₂S20 belong. CaFeSeO contains puckered sheets consisting of FeSe₂O₂ tetrahedra located in the ac plane that are also vertically separated by Ca²⁺ layers oriented parallel to the hexagonal c axis, see FIG. 14. A major reason for the structural difference between SrZn₂S₂O and SrFe₂S₂O may be the electronic configuration of these d transition metal cations. While the Zn²⁺ ion has the closed-shell (spherical) d¹⁰ electronic configuration, tetrahedrally coordinated Fe²⁺ ion possesses a doubly occupied e_(g) orbital, which favors a more distorted coordination geometry. A distortion index (D) defined by Baur is useful for evaluating the magnitude of distortion in polyhedra. D is calculated using bond lengths in a polyhedron, using equation 1, below:

$\begin{matrix} {D = {\frac{1}{4}{\sum\limits_{1}^{4}\left( \frac{{l_{i} - l_{av}}}{l_{av}} \right)}}} & (1) \end{matrix}$

where l_(i) is the length between the metal center and the ith surrounding atom, and l_(av) is the average bond length. A larger D value indicates a higher magnitude of polyhedral distortion. The D value of the FeS₃O tetrahedra in SrFe₂S₂O is 0.08474, much larger than the 0.07400 and 0.07115 for the Zn(1)S₃O and Zn(2)S₃O tetrahedra, respectively, in SrZn₂S₂O. This is consistent with the difference in electronic configuration between Zn²⁺ and Fe²⁺. Note that CaFeSO and CaZnSO adopt similar crystal structures despite the large difference between their D values (0.08609 for FeS₃O and 0.07845 for ZnS₃O). This suggests that the difference in the anion ordered arrangement should be another important factor for maintaining the same crystal symmetry.

The thermogravimetric (TG) analysis of SrZn₂S₂O, shown in FIG. 5, demonstrates a high thermal stability in air, up to 650° C. An irreversible weight increase is observed once the temperature exceeds 650° C. and continues to 1000° C. The TG curve shows a weight gain starting at 650° C. that reaches a maximum value at 970° C. and then decreases on further heating up to 1000° C. The net weight gain is 14.2%. Based on a powder the X-ray diffraction analysis of the products, FIG. 13, the net gain results from the decomposition of SrZn₂S₂O into ZnO and SrSO₄. The calculated weight gain is 16.1%, which is consistent with the experimental value.

The UV-vis-NIR absorption spectrum of SrZn₂S₂O powder is shown in FIG. 6. The absorption curve exhibits a steep increase close to 4 eV, and an extrapolation of the linear portion of the absorption plot to the x-axis indicates a band gap of E_(g)=3.86 eV. The large band gap is consistent with the clear, colorless crystals grown out of the flux. The weak absorption noticeable between 3 and 3.8 eV is likely due to impurity states. The 3.86 eV band gap of SrZn₂S₂O is significantly larger than the 3.3 eV band gap of ZnO₄ as well as the 3.1 eV band gap of SrZnSO and is comparable with those found in zinc-based sulfides and oxysulfides, such as ZnS (3.8 eV), CaZnSO (3.7 eV), and BaZnSO (3.9 eV).

FIG. 7 shows the total and partial DOS and the band dispersion of SrZn₂S₂O, which are qualitatively similar to those of (Ca/Sr)ZnSO with similar local coordination environments around the metal cations. The computationally optimized lattice constants and atomic coordinates are consistent with those determined by the single-crystal XRD analysis, see Table 6. The band dispersion reveals that SrZn₂S₂O is a direct band gap semiconductor with the band gap energy of 2.26 eV at the Γ point. Underestimation of the band gap energy is typical of DFT calculations. The valence band maximum is mainly composed of the O-2p and S-3p states. The S-3p band is located at a higher energy level than the O-2p band, as observed in the other oxysulfide compounds. The partial DOS plots indicate the strong hybridization between Zn-3d/Zn-4s/Zn-4p or Sr-4d/Sr-5s/Sr-5p and O-2p/S-3p states in the valence band ranging from −6 eV to the Fermi energy level, resulting in the (Zn-3d/Zn-4s/Zn-4p)-(O-2p/S-3p) bonding states and the (Zn-3d)-(O-2p/S-3p) antibonding state, see FIG. 15. The conduction band maximum is composed of Zn-4s and the Zn-4p and Sr-4d states that reside at higher energy regions. These states form antibonding states with O-2p/S-3p. Based on these results, the direct band gap corresponds to a transition between S-3p and Zn-4s energy levels.

Materials that crystallize in polar NCS space groups may exhibit SHG behavior, and since SrZn₂S₂O crystallizes in the NCS polar space group Pmn2₁, powder SHG measurements with a 1064 nm laser were performed. FIG. 8 shows the SHG intensities as a function of particle size, which are compared with the known SHG intensity of KDP. The results are consistent with type-I phase-matching, as proposed by Kurtz and Perry. The SHG intensities increase with increasing particle size and reach a plateau at an SHG efficiency of approximately 2 times that of KDP. It should be noted that SrZn₂S₂O is the first example of an oxysulfide material to demonstrate a phase-matching behavior, in contrast to the nonphase matching behaviors in CaZnSO and α-Na₃PO₄S.

Based on the anion group theory described by Chen, dipole moments of anionic polyhedra play a crucial role in the SHG response. Therefore, to evaluate the contribution to the SHG from the asymmetric anionic groups in SrZn₂S₂O, the dipole moments of [SrS₄O₂] and [ZnS₃O] building units in the unit cell were calculated using a simple bond-valence approach proposed by Poeppelmeier. For comparison, the dipole moments in wurtzite ZnS and CaZnSO were also calculated. As detailed in Table 3, see FIG. 9, the magnitude of the dipole moments of SrS₄O₂, Zn(1)S₃O, and Zn(2)S₃O building units are estimated to be 12.342, 4.375, and 3.032 D (Debye: 10⁻¹⁸ esu cm), respectively. Both Zn-centered tetrahedra have a dipole moment much larger than the one observed for ZnS₄ in wurtzite, ZnS, but somewhat smaller than the dipole moment of ZnS₃O in CaZnSO. The dipole moments of Zn(1)S₃O and Zn(2)S₃O tetrahedra point to the S3 triangular planes, similar to what is observed for CaZnSO. Given the mm² point group for SrZn₂S₂O, only the z components of the dipole moments of Sr- and Zn-centered polyhedra contribute to the polarization in the unit cell. The net dipole moments along the polar c axis in the unit cell are 4.695, 2.344, and 2.609 D for SrS₄O₂, Zn(1)S₃O, and Zn(2)S₃O building units, respectively. Because the net dipole moments of Zn(1)S₃O and Zn(2)S₃O tetrahedra are directed antiparallel to each other, the dipole moment of the SrS₄O₂ octahedra appears to be primarily responsible to the SHG response of SrZn₂S₂O.

Understanding the relationship between phase matchability and NCS structures is a challenging subject, especially for nonmolecular solids. Although SrZn₂S₂O and CaZnSO possess similar chemical and electronic structures, the former is phase matching and the latter is non-phase matching. The underlying mechanism of the phase matchability in SrZn₂S₂O is not understood at this point; however, the different anion order and arrangements of the polar anionic units should yield birefringence (Δn) satisfying the phase matching conditions. Recently, Lin et al. discussed the SHG properties of phasematchable AM₃Se₆ (A=Cs, Ba, M=Ga, In, Si, Ge, Sn) and nonphase-matchable CsM₉Se₁₂ (M=0.56Ga/0.44Cd) crystallizing in the polar NCS R3 space group. They suggested that Δn is correlated with the magnitude of the dipole moments in AM₃Se₆, with one type of dipole moment derived from MSe₄. By contrast, in CsM₉Se₁₂, three types of dipole moments of the MSe₄ units are aligned along different directions resulting in small Δn values, which are responsible for the nonphase matching behaviors. The relationship between the orientation and the magnitude of acentric building units and the phase matchability in the selenide phases does not seem to be consistent with that in the zinc oxysulfide phases. In phase matchable SrZn₂S₂O, the dipole moments of SrS₄O₂, Zn(1)-S₃O, and Zn(2)S₃O, which lie in the be plane, are inclined relative to the c axis by −22°, 32°, and −59°, respectively, see FIG. 9 Table 3. The orientation preference of the building units is weaker than for those in the nonphase matchable CaZnSO, where the dipole moments of the CaS₃O₃ and ZnS₃O units are aligned along the c direction. The difference in phase matchability between the selenide and oxysulfide phases may be related to the biaxial structure of SrZn₂S₂O, which cannot simply be compared with the uniaxial CaZnSO and selenide phases. Detailed future examinations of the optical properties of larger sized single crystals combined with theoretical calculations should lead to an improved understanding of the phase matchability in these oxysulfide materials.

Accordingly, single crystals of a new noncentrosymmetric polar oxysulfide SrZn₂S₂O (s.g. P_(mn)2¹) have been grown in a eutectic KF—KCl flux. The oxysulfide has unusual wurtzite-like slabs consisting of close-packed corrugated double layers of ZnS₃O tetrahedra; the slabs are vertically separated from each other by Sr atoms. These structural features are significantly different from the hexagonal AZnSO (A=Ca, Sr, Ba) which contains similar ZnS₃O tetrahedra. SrZn₂S₂O exhibits phase-matching behavior with SHG efficiencies twice that of KDP, which likely results from the presence of the acentric ZnS₃O and SrS₄O₂ anionic units. This is the first realization of a phase matchable oxysulfide material. The large band gap energy of 3.86 eV and the high thermal stability up to 650° C. in an O₂ gas atmosphere is beneficial for practical applications. Understanding of the difference in phase matchability between SrZn₂S₂O and CaZnSO will serve as a guide for the chemical design of additional functional mixed anion materials.

In a further embodiment, crystal growth was achieved via single crystals of SrZn₂S₂O grown from KF/KCl eutectic molten salt. 1 mmol of SrO, 1 mmol of Zn, 1 mmol of S, 3.4 mmol of KF, and 4.1 mmol of KCl were loaded in a silver tube that had been welded on one end. The top of the tube was crimped and sealed in an evacuated silica tube under 10-4 Pa. The starting materials were heated in a tubular furnace to 900° C. at 5° C./min, held for 24 h, and cooled to 600° C. at 0.17° C./min. Then the furnace was turned off and cooled down naturally to room temperature. The product was sonicated in water and isolated via vacuum filtration. Colorless transparent plate-like crystals (typical dimension 0.1′0.2′0.05 mm3. See FIG. 10, which shows a photograph of a colorless transparent single crystal of SrZn₂S₂O., which were characterized as SrZn₂S₂O by single-crystal XRD, were isolated from the filtered product containing ZnS and ZnO crystals.

Polycrystalline powder samples of SrZn₂S₂O were synthesized using SrO, Zn, and S in a stoichiometric ratio. The starting materials were thoroughly mixed in an agate mortar, pressed into a pellet, and heated in an evacuated silica tube 1000° C. for 24 h. Powder XRD measurement using a Bruker D2 Phaser equipped with an LYNXEYE silicon strip detector and a Cu-Kα source identified SrZn₂S₂O as the main phase and SrS as a minor phase. Additional heat treatment on the same condition did not improve the relative amount of SrZn₂S₂O to SrS. Heating at higher temperatures (>1000° C.) decomposed SrZn₂S₂O. The pure sample was obtained by sonicating the product prepared at 1000° C. with water. SrS was easily decomposed by water and removed via vacuum filtration. The powder XRD data of SrZn₂S₂O after washing is presented in FIG. 11, which shows Comparison of the powder XRD pattern of purified SrZn₂S₂O with a theoretical pattern based on the single-crystal XRD analysis. A small amount of SrS was detected.

Rietveld refinement. Synchrotron X-ray powder diffraction (SXRD) data on the purified SrZn₂S₂O powder sample was collected at room temperature using a one-dimensional X-ray detector installed on BL15XU, NIMS beamline at SPring-8 in Japan. The synchrotron radiation X-rays were mono-chromatized to the wavelength of 0.65298 Å. The sample was loaded in 0.2 mm diameter glass capillary, and the diffraction data was recorded in 0.003° increments in the range of 6≤2θ≤50°. As presented in FIG. 12, which shows SXRD patterns for purified SrZn₂S₂O measured at room temperature, the SXRD data was analyzed by Rietveld refinement using the program RIETAN-FP [1]. The refined crystallographic data are given in FIG. 19, see Table 7. With respect to the SXRD patterns for purified SrZn₂S₂O measured at room temperature, obtained, calculated, and difference values are presented by cross marks (red), upper solid lines (black), and bottom solid lines (blue), respectively. The upper and lower vertical lines (green) represent the Bragg peak positions of SrZn₂S₂O and SrS, respectively. SrS is present at 0.3 weight %. FIG. 13 shows room-temperature XRD pattern of the products after TG measurement, which could be assigned to ZnO and SrSO₄. SrZn₂S₂O powder was heated in an aluminum pan up to 1000° C. in O2 gas atmosphere. FIG. 14 shows a comparison of the crystal structure of SrZn₂S₂O (Pmn2₁) with that of CaFeSeO (Cmc2₁). FIG. 15 shows Crystal Orbital Hamiltonian Population (COHP) for (Zn1/Zn2)-O and (Zn1/Zn2)-S interactions in SrZn₂S₂O. FIG. 16 shows Table 4—Atomic coordinates and equivalent isotropic displacement parameters Ueq for SrZn₂S₂O at 300 K. FIG. 17 shows Table 5—Anisotropic displacement parameters Uij (102′Å2) for SrZn₂S₂O at 300 K. FIG. 18 shows Table 6—Lattice constants and atomic coordinates obtained by the first principle calculations for SrZn₂S₂O.

While the present subject matter has been described in detail with respect to specific exemplary embodiments and methods thereof, it will be appreciated that those skilled in the art, upon attaining an understanding of the foregoing may readily produce alterations to, variations of, and equivalents to such embodiments. Accordingly, the scope of the present disclosure is by way of example rather than by way of limitation, and the subject disclosure does not preclude inclusion of such modifications, variations and/or additions to the present subject matter as would be readily apparent to one of ordinary skill in the art using the teachings disclosed herein. 

What is claimed is:
 1. A new zinc oxysulfide compound comprising; a noncentrosymmetric crystalline structure with chemical formula SrZn₂S₂O; lattice parameters of α=3.87440(10) Å, b=9.9847(3) Å, and c=6.0916(2) Å; and corrugated double layers of ZnS₃O tetrahedra vertically separated by Sr²⁺ ions.
 2. The new zinc oxysulfide compound of claim 1, wherein an O/S anion ordered arrangement provides two distinct orientations of the ZnS₃O tetrahedra.
 3. The new zinc oxysulfide compound of claim 1, wherein the compound crystallizes in noncentrosymmetric polar space group Pmn2₁.
 4. The new zinc oxysulfide compound of claim 1, wherein an O/S anion ordered arrangement yields two distinct orientations of the Zn-centered tetrahedra.
 5. The new zinc oxysulfide compound of claim 1, wherein the compound forms colorless, transparent crystals.
 6. The new zinc oxysulfide compound of claim 1, having a band gap of 3.86 eV.
 7. The new zinc oxysulfide compound of claim 1, wherein the compound is stable up to 650° C. in O₂ gas atmosphere.
 8. The new zinc oxysulfide compound of claim 1, wherein the compound is phase matchable with twice a SHG intensity of potassium dihydrogen phosphate (KDP).
 9. The new zinc oxysulfide compound of claim 1, wherein the compound has a Sr:Zn:S molar ratio of approximately 1.0:2.0:2.3.
 10. The new zinc oxysulfide compound of claim 1, wherein the compound has a band gap energy of 3.86 eV.
 11. The new zinc oxysulfide compound of claim 1, wherein temperatures greater than 1000° C. decompose the SrZn₂S₂O compound
 12. A method for synthesizing the compound SrZn₂S₂O comprising: employing a molten salt method using a eutectic KF—KCl mixture; loading a silver tube with 1 mmol of SrO, 1 mmol of Zn, 1 mmol of S, 3.4 mmol of KF, and 4.1 mmol of KCl; placing the silver tube in a silica tube that was evacuated to 10⁻⁴ Pa and sealed; and heating the silver tube in a tube furnace to 900° C. at 5° C./min, held for 24 h, and cooled to 600° C. at 0.17° C./min.
 13. The method of claim 12, further comprising, extracting the compound from flux by dissolving the flux in water followed by sonication.
 14. A method for solid state synthesis of SrZn₂S₂O comprising: mixing SRO, Zn and S in a stoichiometric ratio in an agate mortar to form a mixture; pressing the mixture into a pellet; heating the pellet in an evacuated silica tube at 1000° C. for 24 hours; and sonicating at 1000° C. with water. 